Unified semi-analytical wall boundary conditions for ...

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HAL Id: hal-00691603 https://hal-enpc.archives-ouvertes.fr/hal-00691603 Submitted on 26 Apr 2012 HAL is a multi-disciplinary open access archive for the deposit and dissemination of sci- entific research documents, whether they are pub- lished or not. The documents may come from teaching and research institutions in France or abroad, or from public or private research centers. L’archive ouverte pluridisciplinaire HAL, est destinée au dépôt et à la diffusion de documents scientifiques de niveau recherche, publiés ou non, émanant des établissements d’enseignement et de recherche français ou étrangers, des laboratoires publics ou privés. Unified semi-analytical wall boundary conditions for inviscid, laminar or turbulent flows in the meshless SPH method Martin Ferrand, Dominique Laurence, Benedict Rogers, Damien Violeau, Christophe Kassiotis To cite this version: Martin Ferrand, Dominique Laurence, Benedict Rogers, Damien Violeau, Christophe Kassiotis. Uni- fied semi-analytical wall boundary conditions for inviscid, laminar or turbulent flows in the meshless SPH method. International Journal for Numerical Methods in Fluids, Wiley, 2013, 71 (476-472), pp.Online. 10.1002/fld.3666. hal-00691603

Transcript of Unified semi-analytical wall boundary conditions for ...

Page 1: Unified semi-analytical wall boundary conditions for ...

HAL Id: hal-00691603https://hal-enpc.archives-ouvertes.fr/hal-00691603

Submitted on 26 Apr 2012

HAL is a multi-disciplinary open accessarchive for the deposit and dissemination of sci-entific research documents, whether they are pub-lished or not. The documents may come fromteaching and research institutions in France orabroad, or from public or private research centers.

L’archive ouverte pluridisciplinaire HAL, estdestinée au dépôt et à la diffusion de documentsscientifiques de niveau recherche, publiés ou non,émanant des établissements d’enseignement et derecherche français ou étrangers, des laboratoirespublics ou privés.

Unified semi-analytical wall boundary conditions forinviscid, laminar or turbulent flows in the meshless SPH

methodMartin Ferrand, Dominique Laurence, Benedict Rogers, Damien Violeau,

Christophe Kassiotis

To cite this version:Martin Ferrand, Dominique Laurence, Benedict Rogers, Damien Violeau, Christophe Kassiotis. Uni-fied semi-analytical wall boundary conditions for inviscid, laminar or turbulent flows in the meshlessSPH method. International Journal for Numerical Methods in Fluids, Wiley, 2013, 71 (476-472),pp.Online. 10.1002/fld.3666. hal-00691603

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❯♥ s♠♥②t ♦♥r②

♦♥t♦♥s ♦r ♥s ♠♥r ♦r tr♥t

♦s ♥ t ♠sss P ♠t♦

rr♥ r♥ ♦rs ❱♦ ss♦ts

♠ ♠rt♥rr♥r

♥tr♦t♦♥

rt♥ ♦♥r② ♦♥t♦♥s s ♦♥ ♦ t ♠♦st ♥♥ ♣rts ♦ t♠♦♦t Prt ②r♦②♥♠s P ♠t♦ ♥ ♠♥② r♥t ♣♣r♦s ♥ r♥t② ♦♣ s ❬ ❪ rt ♦♥r② ♦♥t♦♥s r ss♥t s♥ ♥ ♠♥② ♣♣t♦♥s r ♣rs ♦♥ ♦♥ ss rqr s s ♦rs ♦♥ ♦t♥ ♦s ♦r s♦r♥ strtrs t♥ s♥ ①♥s strtr ♥trt♦♥s ♥ ♣♦r♣♥ts t t s ♥♦♦s ♣rrqst t♦ ♠♣r♦ tr♥ ♠♦♥ ♥r s

♥② ♠t♦s ♦r ♠♣♠♥t♥ s♦ s ♥ P ♥ ♦♣♦r t ♣st t♦ s ♠♦♥ t ♠♦st ♣♦♣r ♥ ♦♠♠♦♥② s ♥tr r♦ t♦rs

♣s ♦rs s s ♥♥r♦♥s ♣♦t♥t ❬❪

tt♦s ♣rts ♦r tr♥t② ♦st ♣rts t ♠♣t②r ♦ t r♥ s♣♣♦rt ♥ ♦♥r② t rt ♣rts t♣rsr ♣②s q♥tts s s ♣rssr ♥ ♦t② t♦ ♥♦r♥♦ s♣ ♦r r s♣ ♦♥t♦♥

♠♥②t ♦♥r② ♦♥t♦♥s s ♦♥ rt♦♥ ♦r♠t♦♥♥tr♦ ② sr♠ t ❬❪ r r♥♦r♠③t♦♥ ♦ tqt♦♥s s ♠ t rs♣t t♦ t ♠ss♥ r ♦ t r♥ s♣♣♦rt❲ sr r♥t ♦ ts ♠t♦ ♥ ➓ r ♥tr♥s r♥t

♥ r♥ ♦♣rt♦rs r ♠♣♦② tt ♥sr ♦♥srt♦♥ ♣r♦♣rts

♦ ts ♠t♦s ♥ts ♥ rs ♥♥r♦♥s♣♦t♥t ♦r ♦r♥② srs t ♥trt♦♥ t♥ ♣rs ♦ t♦♠s ♥s s t♦ ♠♦ t r♣s♦♥ t♥ ♣rt ♥ ♦♥r② ♣rts ♠t♦ s s② t♦ ♠♣♠♥t ♥ ♦r ♦♠♣① ♦♠trs ♥ ♦♠♣tt♦♥② ♣ ♦r t s t♦ s♣r♦s ♦r ♦r ♥st♥ t s

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♠♣♦ss t♦ ♠♥t♥ ♣rts ① ♦♥ rt ♥ t ♣rs♥ ♦rt②

tt♦s ♣rts r♦♠♠♥ ♥ ❬❪ ♣r♥ts s ♥♦♥♣②s♦r ♦r t ♣♦st♦♥♥ ♦ ♦st ♣rts ♥ ♦♠♣① ♦♠trs♥ ♣rtr② ♥② ♣rtr② ♥ 3D ♦r♦r t ♦♠♣tt♦♥♦rt rqr s ♥♦t ♥ ♥ tt ♥rs t ♥♠r ♦ ♣rtst♦ t ♥t♦ ♦♥t ♥ t srt s♠♠t♦♥s ♥

♥② t s♠♥②t ♣♣r♦ s ttrt t♥s t♦ ts rt♦♥rt♦♥ ♠♥s tt s♦♠ ♣②s q♥tts s s ♠♦♠♥t♠ t♦♠t② ♦♥sr ❯♥♦rt♥t② t ♦r♥ tt♠♣t ♥♦t ♣rs♥t r ♥ s♠♣ ② t♦ ♦♠♣t r♥♦r♠③t♦♥ tr♠s ♥tr♦ rtr♠♦r t ♦r♠t♦♥ ♣r♦♣♦s s ♥♦t t♦ r♣r♦ ②r♦stt ♣rssrs ♦r t♦ t ♥t♦ ♦♥t t sr strss ♦♥

s ♣♣r tr♦r ts t s♠♥t② ♣♣r♦ ♦ ❬❪ ♥ ①t♥st s♦ tt t r② ♦ t ♣②s s s t ♣rssr ♥①t t♦ ss ♦♥sr② ♠♣r♦ ♥ t ♦♥sst♥t ♠♥♥r ♦♣ ♦r ♦rrt♦♣rt♦rs ♦s s t♦ ♣r♦r♠ s♠t♦♥s t tr♥ ♠♦s s ♦r ♣rs♥t tr ② ♥s

• t♠ ♥trt♦♥ s♠ s ♦r t ♦♥t♥t② qt♦♥ rqrs ♣rtr tt♥t♦♥ ♥ s r② ♠♥t♦♥ ② ❱ ❬❪ ♣r♦ tr s♥♦ ♣♦♥t ♥ s♥ ♣♥♥ ♥ t♠ ♦ t ♣rts ♥st② ♥♦ r♥r♥t ♦rrt♦♥s r s ② s♥ ♥r♦♥r② r♥♦rrt rs♦♥ ♦ t t♠ ♥trt♦♥ s♠ ♦ t ♦r♠ ♣r♦♣♦s ♥❬❪ ♦♥t♠ s♠t♦♥s ② st ♦r tr♥t ♦s ♥ t ♦♥t①t♦ rt ♦♥r② ♦♥t♦♥s r ♣♦ss

• ♦ ♦♠♣t t r♥ ♦rrt♦♥ ♠♥ ♥ ♦♥t ❬❪ s ♥ ♥②t s ♦♠♣tt♦♥② ①♣♥s rs sr♠ t

❬❪ ♥ t ❬❪ s ♣♦②♥♦♠ ♣♣r♦①♠t♦♥ ♥ t t♦ ♥ ♦r ♦♠♣① ♦♠trs ❲ ♣r♦♣♦s r t♦ ♦♠♣tt r♥♦r♠st♦♥ tr♠ ♦ t r♥ s♣♣♦rt ♥r s♦ t ♥♦t♠ ♥trt♦♥ s♠ ♦♥ s ♥② s♣ ♦r t ♦♥r②

• ♦♥r② tr♠s ss r♦♠ t ♦♥t♥♦s ♣♣r♦①♠t♦♥ r ♥② sr s♠♠t♦♥s ♦♥② rqr ♥♦r♠t♦♥ r♦♠ ♠s ♦ t ♦♥r② t♥q ♦♣ r ♦s s t♦ ♦rrt t♣rssr r♥t ♥ s♦s tr♠s ♥ ♥ ♣r♦ ♣②s② ♦rrtsr strss s♦ tt ♥ t s♦♥ qt♦♥ ♦ sr q♥tt②♥ s♦ rt② s♥ P s s t tr♥t ♥t ♥r②♦r ts ss♣t♦♥ ♥ k − ǫ ♠♦ ♦ tr♥

s ♣♣r s ♦r♥s s ♦♦s ♥ t ♥①t t♦♥ ♥tr♦ t ♦r♠t♦♥s ♦r ② ♦♠♣rss P ♥tr♦♥ t s srtst♦♥s ♦r♦♣rt♦rs s♦s ♦rs ♥ tr♥ ♠♦♥ ♥ t t♦♥ ♦♦♥ t♥ ♦♣ t ♦♥sst♥t ♦♥r② ♦♥t♦♥s t ♠♣r♦ t♠ ♥trt♦♥ ♥ ♣♦st♦♥♣♥♥t t♥q t♦ ♦♠♣t t ♥st② ♣♣rt♥ ♣rs♥ts t ♦♠♣tt♦♥ ♦ t r♥♦r♠③t♦♥ tr♠s s♥ ♥♦ t♠♥trt♦♥ s♠ ♦r ♣rs♥t♥ t ♥♥ ♦r ♥ t t♦♥ ♦♥♥♠r rsts

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s P ♦r♠t♦♥s ♦r ② ♦♠♣rss

t♦♥♥

♦♥srt ♦r♥♥ qt♦♥s

st② ♦♠♣rss t♦♥♥ s ♠♦ ② st ♦ ♣rts ♥♦t ② t ssr♣ts (.)a ♥ (.)b ♥ ♦♠♥ Ω st ♦ t ♣rts s ♥♦t ② F r ♣rt a ∈ F ♣♦sssss ♥♦r♠t♦♥ ss ts ♠ss ma ss♠ ♦♥st♥t ts ♣♦st♦♥ ra ts ♦t② ua t r♥♥ rt ♦ t ♣♦st♦♥ ts ♥st② ρa ts ♦♠ Va = ma

ρa

♥ ts♣rssr pa s♣t srt③t♦♥ s s ♦♥ t♥ ♥tr♣♦t♦♥ ♦rr♥ ♥t♦♥ w, t ♦♠♣t s♣♣♦rt Ωa t♥ rrs t♦ t s♣♣♦rt ♦ tr♥ ♥t♦♥ ♥tr ♦r ra ♦ rs R ❲ ♥r② ♥♦t ② t ssr♣ts(.)ab t r♥ ♦ q♥tt② t♥ t ♣♦st♦♥s a ♥ b ♦r ♥st♥uab ≡ ua − ub ♥ rab ≡ ra − rb ♦ ①♣t♦♥s r ♠ t t ♦♦♥♥♦tt♦♥s wab ≡ w (rab) ♥ ∇wab ≡ ∇aw (rab) r t s②♠♦ ∇a ♥♦tst r♥t t t ♣♦♥t ra

❲t ts ♥♦tt♦♥s ♦♠♠♦♥② s ♦r♠ ♦t ♦♥t♥t② qt♦♥ s s ❬❪

dρa

dt=∑

b∈Fmb∇wab.uab

r ddt

♥♦ts t r♥♥ rt tt s t♦ s② t rt ♦♥t ♣rt ♣t t ♥ r r♦♠ t ♦♦♥ ♥t♦♥ ♦ t ♥st②

ρa =∑

b∈Fmbwab

♥s ♠♦♠♥t♠ qt♦♥ ♥ rtt♥ s ♦♦s

dua

dt= −

b∈Fmb

(pa

ρ2a

+pb

ρ2b

)∇wab + g

r g s rt② qt♦♥ ♦ stt ♥s ♥st② ♥ ♣rssr

pa =ρ0c

20

γ

[(ρa

ρ0

− 1

]

r ρ0 s t rr♥ ♥st② ♦ t c0 s t s♣ ♦ s♦♥ ♥ γ = 7s ♥r② ♦s♥ ♦r tr

❱s♦s ♦rs

s♦s tr♠ s s ♥ ts ♦r ♥ P ♦r ♦♠♣t♥ t s♦s tr♠1

ρ∇. (µ∇u) s t♦ ♦rrs t s ❬❪

1

ρa

∇. (µ∇u)a =∑

b∈Fmb

µa + µb

ρaρb

uab

r2ab

rab.∇wab

t r♥t ♦♣rt♦r s ♥ ② ∇a ≡ ex∂

∂xa

+ ey∂

∂ya

+ ez∂

∂za

(ex, ey , ez) ♥

t ss t♦r tr ♦ t rts♥ ♦♦r♥t s②st♠ ♥ 3D

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r t ②♥♠ s♦st② µ s ♥ ②

µ ≡ νρ

♥ ν s t ♥♠t ♠♦r s♦st②

♣rt♦r ♥t♦♥s ♦r tr ♥②ss ♥ srt ♦♣rt♦rs r♥t GradaAb r♥ DivaAb ♥ ♣♥ Lapa (Bb, Ab)♦ rtrr② srt sr Ab ♥ Bb ♦r t♦r s Ab s

GradaAb ≡ ρa

b∈Fmb

(Aa

ρ2a

+Ab

ρ2b

)∇wab

DivaAb ≡ − 1

ρa

b∈FmbAab.∇wab

Lapa (Bb, Ab) ≡ ρa

b∈Fmb

Ba + Bb

ρaρb

Aab

r2ab

rab.∇wab

r Aab ≡ Aa − Ab ② r ♣♣r♦①♠t♦♥s ♦ t ♦♥t♥♦s r♥tr♥ ♥ ♣♥ ♦♣rt♦rs rs♣t② ♥♦t ② ∇a ∇. ♥ ∇.∇s t qt♦♥ ♦ ♦♥t♥t② ♥ t ♠♦♠♥t♠ qt♦♥ ♥ rrtt♥ s ♦♦s

dρa

dt= −ρaDivaub

dua

dt= − 1

ρa

Gradapb + g +1

ρa

Lapa (µb, ub)

♦♣rt♦rs Grada ♥ Diva r s t♦ s♦♥t t s ♣♦ss t♦♥ r♥ts ♦ ts tr ♦♣rt♦rs ♦♥sr♥ ts ♣r♦♣rt② ♦ ♥t♦♥s ❬❪

r♥ ♠♦♥ ♥ P

②♥♦s ♣♣r♦ ♦♥ssts ♥ ♦♥sr♥ ♦♥② t ♠♥ ♣rt ♥♦t ②u ♦ t ♦t② u ♥ t qt♦♥ ♦ r t♦s t♥ ♠♦♥ tts ♦ t tt♥ ♣rt ♦ t ♦t② ♦♥ t ♠♥ ♦t②

k− ǫ tr♥ ♠♦ ♦♣ ② ♥r t ❬❪ t♦ tr♥s♣♦rt qt♦♥s ♦ k t tr♥t ♥t ♥r② ♥ ǫ ts ss♣t♦♥ t♦ t♠♦♠♠t♠ qt♦♥ s ♠♦ s ♦♦s

Dρa

Dt= −ρaDivaub

Dua

Dt=

1

ρa

Gradapb + 23ρkb + Lapa (µb + µTb, ub) + g

Dka

Dt=

1

ρa

Lapa

(µb +

µTb

σk

, kb)

+ Pa − ǫa

Dǫa

Dt=

1

ρa

Lapa

(µb +

µTb

σǫ

, ǫb)

+ǫa

ka

(Cǫ1Pa − Cǫ2ǫa)

♥ t st♦st ♣♦♥t ♦

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r t rtD

Dt≡ ∂

∂t+ u.∇ s t r♥♥ rt ♦♥ t

②♥♦s r ub k − ǫ ♠♦ ♥s t tr♥t ♥ts♦st② νT ≡ µT

ρt♦ t tr♥t ♥t ♥r② k ♥ ts ss♣t♦♥ ǫ ②

νTa = Cµ

k2a

ǫa

t ♦♥st♥ts σk σǫ Cǫ1 ♥ Cǫ2 ♥ ② ❬❪

♣r♦t♦♥ tr♠ ♦ k Pa s ♥ ②

Pa = νTaS2a

r S2a ≡ 2Sa : Sa s t sr ♠♥ rt♦str♥ t♥s♦r str♥ rt

♦ t ♠♥ ♦t② s ♥ ② Sa ≡ 12

(∇au + ∇au

T) ❱♦ ♥ ss

❬❪ srt③ ♥ t P ♦r♠ t ♦t② r♥t

Gradaub ≡ − 1

ρa

b∈Fmbuab ⊗ ∇wab

♥ t ♦♦♥ ♦r s ♦ s♠♣t② r♦♣ ♦rrs t♦ ♥♦t

♦t② ♥ ♣rssr ♥ ts ♥♦t r♥♥ rtsd

dt rr

s♦ ♣ ♥ ♠♥ tt ♥r tr♥t ♦♥t♦♥s t ttr q♥tts r♦♥sr s ②♥♦sr ♥ t r♥♥ rt s ♦♥ t②♥♦s r ♦t②

♦♥r② ♦♥t♦♥s ♥ rt t♠

st♣♣♥

rt♦♥ ♦ ♦♥r② tr♠s s♥ ♦♥t♥♦s

♥tr♣♦t♦♥

sr♠ t s r♥♦r♠st♦♥

♥st ♦ ss♠♥ tt ρa ≃∑

b∈Fmbwab ♥rst♠ts ρa ♥ t

♣rt a s ♦s t♦ ♦♥r② s r sr♠ t ❬❪ r♥♦r♠s t st♠t♦♥ s♥ ♥t♦♥ γa

ρa ≃ 1

γa

b∈Fmbwab

r γa s ♥ ②

γa ≡∫

Ω∩Ωa

w (r′ − ra) dV ′

♥ ♥r γa s ♥ r♥ ♣♥♥ ♦♥② ♦♥ t ♣♦st♦♥ ♦ t♣rt a t rs♣t t♦ ♦♥rs ♦ Ω r r♦♠ s♦ ♦♥r② γa = 1.

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b ab R

Ω

Ωa

γa

∂Ω

r r♥♦♥r② ♥trt♦♥

♥tr♦t♦♥ ♦ γa ♥t♦ t rt♦♥ ♦ t ♦r♥♥ qt♦♥s st♦ s♦♠ ② r♥s s s t ♥ ♦♥t♥t② qt♦♥ ❬❪ r strt♥r♦♠ s rrtt♥

dρa

dt=

1

γa

b∈Fmb∇wab.uab −

ρa

γa

∇γa.ua

s ♥ ♦♠♣r t ♦r♥② t r♥t ∇γa s ♥ ②

∇γa ≡∫

Ω∩Ωa

∇aw (r′ − ra) dV ′ =

∂Ω∩Ωa

w (r′ − ra)ndS′

r t s♦♥ ♥tr s ♦t♥ s♥ t ss t♦r♠ ♥ r n st ♥r ♦♥r② ♥♦r♠

♥ ♦rr t♦ t t ♥ ♥tr♥ ♦rs ♥ ♦♥tt ♦rs sr♠t ❬❪ r t ♥tr♥ ♥r② s♥ t qt♦♥ ♦ r♥ ② ♦t♥ ♥ ♥tr♥ ♦r t♦ t ♣rssr ♦rrt♦♥ ♦ sr♠ t

♥ ①♣rss ♥ tr♠s ♦ ♥ ♦♠♣t ♥ rt♦♥ s♥s ♦♣rt♦rsr♥t ♥ r♥ ♥ ♦♥ ♥ ♥

GradKa Ab ≡ ρa

b∈Fmb

(Aa

γaρ2a

+Ab

γbρ2b

)∇wab −

Aa

γa

∇γa

DivKa Ab ≡ − 1

γaρa

b∈FmbAab.∇wab +

1

γa

Aa.∇γa

s t ♦♣rt♦rs r② t s♦♥t♦♥ ♣r♦♣rt② ♥ rt♦♥s st ♦s ts ♣r♦♥ t ♦♥sst♥② t♥ t ♠♦♠♥t♠ qt♦♥ ♥ t ♦♥t♥t② qt♦♥ ♥ tr♠ ♦ GradK

a Ab s s② sr♠ t s ♦♥r② ♦r ♥ t ♦♦♥ ♣r♦♣♦s ♥♥♥ ♦r♠ ♦ t ttr ♠♦ ♥ ♠♦r rt r♣rs♥tt♦♥ ♦r♥ts ♦♥ t

♥r s♣ ♦ t ♦♥r②

♦r ♦♥rs ♦ rtrr② s♣ tr s♣ ∂Ω ♦ t ♦♠♥ Ω, s ♣♣r♦①♠t t strt s♠♥ts ♥ 2D ♥♦t ② t ssr♣t (.)s

Page 8: Unified semi-analytical wall boundary conditions for ...

b aR

e1

e2Ss

ns

♦♥r② t s♠♣rts e ♥ r♥ ♥ ts♠♥ts s sr Ss ♥ ♥ ♥r ♥♦r♠ns

e

θ

e e

t ♦ t ♦♠ ♦ ♥ ♣rt

r ♦♥r② ♣r♦♣rt② ♥t♦♥s

♥♦r♠ ns ♥ sr r Ss s r st ♦♥t♥♥ ts♠♥ts s ♥♦t ② S s♠♥t s ♥ ② t♦ ♣♦♥ts ♥♦t② t ssr♣t (.)e1 ♥ (.)e2 ♥ ♥t ♦♠ Ve ♥ ② Ve = me

ρ0

r ρ0 s rr♥ ♥st② ♥t ♦♠ ♦ ♣rts s rt♦♥♦ t ♥t ♦♠ ♦ ♣rts Vf ♦r ♥st♥ ♦r ♣♥ Ve = 1

2Vf

♦r ♥r② ♦r ♥ ♣rt ♦♥ t ♥ ♥ θ s♣② ♦♥t r Ve = θ

2πVf

st ♦♥t♥♥ t ♣rts s ♥♦t ② E s ♣rtss♦ s♠ ♣rts ♥ ts rt r ♦ ♣rtr ♥trst ♦r r♦r♥t ♣rssr t t s♦ ♦♥r② ♥ ♥ ♦r ♥ strtr ♦♣♥ ♦r ①♠♣ ② r s♦ s t♦ ♠♣r♦ r② ♦ t ♦♥t♥t②qt♦♥ s t② ♠♠ t t s ♠♣♦rt♥t t♦ ♥♦t tt t② rt♥ ♥t♦ ♦♥t ♥ t ♦♥t♥t② qt♦♥ ♥ ♥ t ♠♦♠♥t♠ qt♦♥ E ⊂ F ♥ t② r r♥ ♣rts tt s t♦ s② t② r ① t s ♠♦t♦♥ss ♥ ♦s ♥♦t ♣♥ ♦♥ t ♠♦♠♥t♠ qt♦♥

①t ♥ t ♦♥trt♦♥ ♦ t s♠♥t s ♥ t ♦ ∇γa t♦

∇γas ≡(∫

re2

re1

w (r) dl

)ns

♥ t♥ ∇γa ♥ ♦♠♣♦s ♥

∇γa =∑

s∈S∇γas

sr♣t♦♥ ♦ t ♦♥r② ♦♠tr② ♥ ①t♥ t♦ 3D ② ssttt♥ t s♠♥ts ② tr♥s ♥ ts s ts ♦♠ Ve ♦ ♣rts♦ s t s♦ ♥ ♦ t

❲ ♦rrt r♥ts

♠♥ s♥t ♦ ♣r♦s t♥qs t♦ t ∇γa s tt t r

♥t ♦♣rt♦r ♥ ② s ♥♦t rt ♥r ♦♥r② ♦r t rsr♥ ♥ s tt r♥ts ♦ ♦♥st♥ts r ♥♦♥ ③r♦ s♠t ♥♦r♠ ♦r♣rssr ♥ ♣r♦ ♣♣ t♦t ♥② ♦② ♦r t r♥t

Page 9: Unified semi-analytical wall boundary conditions for ...

♦ t ♣rssr s ♥♦t ③r♦ r②r ♥ ♣rts rrr♥ t♠ss sr ♦ ♦rrt tt ♥ ♦ t♦ t ♦♥t♥♦s ♥tr♣♦t♦♥♦ ♥ rtrr② ♥tr ♥t♦♥ f t ♣♦♥t r

〈f〉 (r) =1

γ (r)

Ω∩Ωr

f (r′) w (r) dV ′

r r ≡ |r − r′| ♥ Ωr s t r♥ s♣♣♦rt ♥tr ♥ r ② ♥tr♣♦t♥t r♥t ♦ t ♥t♦♥ f ♥ t s♠ ② t ♦♠s

〈∇f〉 (r) = − 1

γ (r)

Ω∩Ωr

f (r′) ∇w (r) dV ′

− 1

γ (r)

∂Ω∩Ωr

f (r′) w (r)ndS′

r t rt♥s s ♦t♥ ② ♥ ♥trt♦♥ ② ♣rts ♥ n s t♥r ♥♦r♠ ♦ t ♦♠♥ t t ♣♦st♦♥ r′ ♥ ♥ s tt t♦♥r② ♦♥t♦♥s ♣♣r ♥tr② tr♦ t s♦♥ ♥tr ♦

♦r♦r ♦♥sr tt t r♥t ♥ ② s srt ♣♣r♦①♠t♦♥ ♦ t ♦♥t♥♦s r♥t ∇f ≡ ρ∇

+ fρ∇ρ t♦ ♦t♥ s②♠♠tr

♦r♠t♦♥ ♦t♥ s s♦ ❬❪

〈∇f〉 (r) ≃⟨

ρ(r)∇f

ρ+

f

ρ(r)∇ρ

⟩(r)

= − 1

γ (r)

Ω∩Ωr

[f

ρ(r′) ρ (r) +

f

ρ(r) ρ (r′)

]∇w (r) dV ′

− 1

γ (r)

∂Ω∩Ωr

[f

ρ(r′) ρ (r) +

f

ρ(r) ρ (r′)

]w (r)ndS′

♥ ♥ t ♦♥r② ♦♥t♦♥s ♣♣r ♥tr② ♥ ♥ ♥♦ stt ♦♦♥ srt ♦♣rt♦r r♥t ♦r ♥ rtrr② Ab s

GradaAb ≡ ρa

γa

b∈Fmb

(Aa

ρ2a

+Ab

ρ2b

)∇wab −

ρa

γa

s∈S

(Aa

ρ2a

+As

ρ2s

)ρs∇γas

♠t♦ t♦ ♦♠♣t ∇γas sss ♥ ➓ rs t ♦♠♣tt♦♥ ♦ ρs ♥ As ♥stt ♥ t ♣rr♣ ♦♥ ②♥♠ ♦♥r②♦♥t♦♥s ♦t tt t srt r♥t rs r♦♠ sr♠t s ♥ ② ♦♥② ♥①t t♦ ♦♥r② ♠♥s tt ♦♥srt♦♥♣r♦♣rts r st r r♦♠ t s

t s ♥♦ ♦rrt s♥ t s♠ t P r♥t ♦ t♦r ♣♣rs ♥ t ♦t② r♥t ♦r ♥st♥ ttr q♥tt②♣②s ② r♦ ♥ t k − ǫ tr♥ ♠♦ s t s rs♣♦♥s ♦r t ♣r♦t♦♥ ♦ ♥t ♥r② ♥ t t tt ♥ ♥♥ ♦ t str♥ rts t rst ♥ t ♥t② ♦ t ♦♥r② t s ♠♣♦rt♥t t♦ rt ♥ts r s ♦r♠ ♥s t♦ ♦rrt t rs♣t t♦ t ♦♥rs♥ tt t t♥s t♦ ♥rst♠t t str♥ rt ♥①t t♦ ♦ ♦rrttt ♣r♦♣♦s ♥ s♠r ② s

Gradaub = − 1

γaρa

b∈Fmbuab ⊗ ∇wab +

1

γaρa

s∈Sρsuas ⊗ ∇γas

Page 10: Unified semi-analytical wall boundary conditions for ...

X(m)

Z(m

)

0 0.05 0.1 0.15

0

0.05

0.1

0.15

0.2

P(Pa)

5500050000450004000035000300002500020000150001000050000

sr♠ t s r♥t ♦♣rt♦r s ♥ t♦ ♠♥t♥ ♥♦r♠ ♣rssr Prts ♠♦ t♦♥ ♥♦♥♣②s qr♠

X(m)

Z(m

)

0 0.05 0.1 0.15

0

0.05

0.1

0.15

0.2

P(Pa)

5500050000450004000035000300002500020000150001000050000

♣rs♥t r♥t ♦♣rt♦r s t♦ ♠♦st ♠♥t♥ ♥♦r♠ ♣rssr s ♥ qr♠

r ♦♠♣rs♦♥ ♦ r♥t ♦♣rt♦rs ♥ ♥ ♥ ♦r♣rssr③♣r♦ ♣♣

♥ t t ♦rrt ♦♠♣♦♥♥ts t str♥ rt S s ♦♠♣t ♦r♥t♦ t ♥t♦♥ ♥ ②

♣♥

♣♥ rst♥ r♦♠ t ♦rrs ♠♦ ♥ s♥ s srtst♦♥ ♦ t ♦♥t♥♦s ♥tr♣♦t♦♥ 〈∇.µ∇f〉 (r) r f s t ♦♥t♥♦ssr ♥ µ t ♦♥t♥♦s s♦st②

〈∆ (µ, f)〉 (r) ≡ 〈∇.µ∇f〉 (r) = 〈∇r′ . [(µ∇f) (r) + (µ∇f) (r′)]〉 (r)

= − 1

γ (r)

Ω∩Ωr

[(µ∇f) (r) + (µ∇f) (r′)]∇w (r − r′) dV ′

− 1

γ (r)

∂Ω∩Ωr

[(µ∇f) (r) + (µ∇f) (r′)] .nw (r − r′) dS′

♦♠♥ t t ♥t r♥ ♣♣r♦①♠t♦♥

∇f(r). (r − r′) ≃ (f(r) − f(r′)) ≃ −∇f(r′). (r′ − r)

s ♥ ➓ t ♦♥r② tr♠s ♣♣r ♥tr② ♥ t s♦♥ ♥ ♦ r♦♠ ♥ ♥trt♦♥ ② ♣rts ♥ n s t ♥r ♥♦r♠ ♦ t ♦♠♥t t ♣♦st♦♥ r′ ❲ ♦♥trt♦♥s ♥s ♥ t ♣♦st♦♥ r s r r♦♠t ♦♥r② s♥ t r♥ w s ♦♠♣t s♣♣♦rt s t ♣r♦♣♦s♦rrt ♣♥ ♦♣rt♦r s

1

ρa

Lapa (Bb, Ab) =1

γa

b∈Fmb

Ba + Bb

ρaρb

Aab

r2ab

rab.∇wab−1

γaρa

s∈S(Bs∇As + Ba∇Aa) .∇γas

s♠ s st ♦s t ♥ rtrr② t♦r Ab ♥ s s

t♦ ♦rrt t s♦♥ tr♠ ♥ t rt♦s qt♦♥

Page 11: Unified semi-analytical wall boundary conditions for ...

❲ ♦rrt ♦♣rt♦rs ♥ t srt rt♦s

qt♦♥s

②♥♠ ♦♥r② ♦♥t♦♥s ♦♥ t ♣rssr

r♥t ♦♣rt♦r ♣♣ t♦ t ♣rssr s

Gradapb ≡ ρa

γa

b∈Fmb

(pa

ρ2a

+pb

ρ2b

)∇wab −

ρa

γa

s∈S

(pa

ρ2a

+ps

ρ2s

)ρs∇γas

♥ r t t♦ ♦♠♣t t ♣rssr ps ♥ t ♥st② ρs ♦♥ t ♥♦s ♥ ♥ r r♦st ② t rst ♦rr ②♥♠ ♦♥t♦♥ s∂ρ∂n

= 0 s ♦♥t♦♥ s ♦♥sst♥t t t r♥♦r♠③t♦♥ ♦♥ ♥ qt♦♥ ♥ t ♣rs♥ ♦ rt② ♥ ♠♦t♦♥ t ♥♦♦s ♦♥t♦♥ ♦♥ t♣rssr s rtt♥ s

∂n

(p⋆

ρ+

u2

2

)= 0

r p⋆ ≡ p − ρg.r ♥ u s t ♠♥t ♦ t ♦t②

♦ ♦♠♣t t ♣rssr ♥ t ♥st② t t ♥ P ♥tr♣♦t♦♥♥ s ♦r t ♣rts ♥ E t ♦ ♠ s t♦ r ♥ s♣t♦

ρe =1

αe

b∈F\EVbρbwbe

pe

ρe

=1

αe

b∈F\EVb

(pb

ρb

− g.rbe +u2

b − u2e

2

)wbe

r t st F \ E ♥♦ts ♣rts F ①♥ ♣rts ♥ E ♥r αe s ♥ ②

αe ≡∑

b∈F\EVbwbe

sr♣t♦♥ ♦ t ♣r tr αe s ♥ ♥ ➓ s qt♦♥

r t s ♠♣♦rt♥t t♦ ♥♦t tt t ♥tr♣♦t♦♥ ♦♥ s s ♦♥ ♣rts ♥ F ♦ ♥♦t ♦♥ t♦ t st ♦ ♣rts E ♦r s♠♣t② r♠♥ ♥ 2D ♥ ♥ t ♥st② ♥ t ♣rssr t t ♠♥ts st♦

ρs =ρe1 + ρe2

2ps

ρs

=pe1/ρe1 + pe2/ρe2

2

r t ♥♦s ♦r ♣rts e1 ♥ e2 r ♥ ♥ ➓ sstrt② t♦ t q♥tts t t rs t♦ ♦♠♣t t sr strss ♥ ➓ ♥ s♦ t ♦ sr tr♥s♣♦rt ② t ♦♥ ♣♣♥① r s ♥♦ t♦rt rstrt♦♥ t♦ t s♣♥ ♦ t ♥♦s

Page 12: Unified semi-analytical wall boundary conditions for ...

❲ sr strss

♦rrt ♦r♠ ♣♣ t♦ t u s

1

ρa

Lapa (µb, ub) =1

γa

b∈Fmb

µa + µb

ρaρb

uab

r2ab

rab.∇wab−1

γaρa

s∈S|∇γas| (µa∇ua + µs∇us) .ns

♥ s♦ s ♥ ♣ ♦ Lapa ♥

♦♥r② tr♠s r t♥ trt s♥ t rt♦♥ ♦t② uτ ♥②

µ∂u

∂n

∣∣∣∣wall

≡ ρuτuτ

r♣rs♥ts t sr strss t t ♥ t ♣rs♥t rt ② ♦♥♥t♦♥ uτ s ♦s♥ t♦ t s♠ rt♦♥ s t ♦ ♦t② s t♥r♣s (µ∇u)s .ns ♥ t ♦♥r② tr♠ ♦ s ♥ ss ♥t ♠♥t♦r ♥t ♦♠ rt♦s ♦s

(µ∇u)a .ns ≃ ρuτsuτs

♦♠♣tt♦♥ ♦ t rt♦♥ ♦t② ♥ ♠♥r s rt♦♥♦t② uτ s q♥tt② ♥ t t ♦♥r② ♦ ♦♠♣t t ♥ ♦♠♣tt♦♥ ②♥♠ ♦ ♥st ♦ s♥ ts ♥t♦♥ s②t t ♥t ♦ ♥♦♥ t ♣②s ♦r ♦ t ♦t② ♥ t♥t② ♦ t ♦♥r② ♦r ①♠♣ ♥ ♠♥r tst s t ♦t② ♣r♦ s ①♣t t♦ ♥r ♦s t♦ t ♥ t♥ t ♦♦♥ rt♦♥s♣t♥ st♥ t♦ t z ♥ ♦t② ♦♥ t u ♦s

uτuτ = limz→0

νu

z

♠♥ ♥t s tt ♦ ♥♦t ♥ t♦ st♠t t rt ♦t ♦t② ♥①t t♦ t r t s t t♦ ♦♠♣t ♥♦tr♥t s tt ♥ ①t♥ t ♥t♦♥ ♦ t rt♦♥ ♦t② ♥ t rr ♣rts ♥trr t t ♦♥r② tt s ♥ t r♥ s♣♣♦rt♥trsts t s ♥ ♥

uτauτa =νua

za

r za s t st♥ t♦ t ♦r ♣rt a

♥t② t♦ t ρsuτsuτs s ♥ t ♦♥t♥t② ♦ strsss t♦ sts

ρeuτeuτe =1

αe

b∈F\EVbρbuτbuτbwbe

♥ rhosuτsuτs s t r t♥ t ♣rts e1 ♥ e2 ♥♥ ➓ s ♦r♠ r s♠r t♦

s♠ trt♠♥t s ①t♥ t♦ tr♥s♣♦rt qt♦♥ ♦ sr ss k ♦r ǫ ♥ t k − ǫ tr♥ ♠♦ ♥ t ♣♣♥①

Page 13: Unified semi-analytical wall boundary conditions for ...

♦♥srt♦♥ sss t♠ ♥trt♦♥ ♦r t ♦♥t♥

t② qt♦♥

♦r♥ t♠ ♥trt♦♥ s♠ s ♥ ♣r♦s ♦r ❬❪ ❬❪ s s♠♣rst♦rr s②♠♣t s♠ r ♥ ♠♣t ♦t② s s ♥ t♣t s ♦ t ♣♦st♦♥ ♥ ♥st②

un+1a = un

a − δt

ρna

Gradnapn

b + g

rn+1a = rn

a + δtun+1a

ρn+1a = ρn

a + δt∑

b∈Fmb∇

nwab.un+1ab

r t s♣rsr♣t (.)n rrs t♦ t t♠ st♣ n ♥ t♦ t t♠ t =

n∑

i=1

δt

♥ ts s♠♠♣t s♠ t ♦ts r ①♣t rs t ♣♦st♦♥sr ♠♣t ♥ t ♦♥t♥t② qt♦♥ ♣♦st♦♥s r ①♣t rs t ♦ts r ♠♣t ♦r ts rs♦♥ ♦ ♥♦t rt t rs ♦ qt♦♥ s ρaDiv ub

♠♣r♦♥ t t♠ ♥trt♦♥ ♦ t ♦♥t♥t② q

t♦♥

♦ ♣t t ♣r♦s t♠ ♥trt♦♥ s♠ t♦ t ♠t♦ ♦ sr♠t ♥ t ♣rs♥t ♠♦ ♦♥ t ♦♦♥ s♠ s ♣♦ss

un+1a = un

a − δt

ρna

Gradn

apnb + g

rn+1a = rn

a + δtun+1a

ρn+1a = ρn

a +δt

γna

[∑

b∈Fmb∇

nwab.un+1ab − ρn

a∇nγa.un+1

a

]

r t ♦♣rt♦r Grada s tr ♦r ①♣r♥ ♦ t t♦rss s♦♥ ts ♣♣r♦ s♠s t♦ stst♦r② rsts ♦r ♠ r s♥ s♥ r t s♦ s r ♣t ♠♣r♠ t rt② s♠t♠ st♣ ♦r ♥ r♥♥♥ ♦♥t♠ s♠t♦♥s ♥ ♥♥ t rt② r t♠ st♣ ♣rts ♥r t ♠♦ rt② ♦♥rss♦② ♥ ♥t② ♣ss tr♦ t ♦♥r② s s ♥ r rt② t♠ st♣ s st ② rs♥ t ♥♠r s♣ ♦ s♦♥ c0

♣r♦♠ s s ② t ♦♥t♥t② qt♦♥ ♥ ♣rts ♥r t♦♥r② r ♦st♥ ♠♦♥ ♥ ♦rt tr ♥sts rs♥ t♥ t ♣rssr rt t♦ t ♥st② ② t qt♦♥ ♦ stt ♦♠s♥s♥t t♦ rt r♣s ♦r t♦ ♥ t ♦tr ♦rs

♦r♥ ♦ ts ♣♥♦♠♥♦♥ s t tr♠ δtγn

a

ρna∇

nγa.un+1a ♥ t t♠

srt③ ♦♥t♥t② qt♦♥ ♥ ♦♥sr s♥ ♣rt♠♦♥ t♦rs t t♥ t t♠s tn ♥ tn+1 r♦♠ t st♥ zn

t♦ zn+1 t ①t rt♦♥ ♦ t ♥st② s ♥♦t r♣r♦ ② t srt

Page 14: Unified semi-analytical wall boundary conditions for ...

X(m)

Z(m

)

0 0.10

0.2

0.4

0.6

0.8

1

P(Pa)

100009000800070006000500040003000200010000

Pr♦s t♠s♠ tc0 = 20m.s−1

X(m)

Z(m

)

0 0.10

0.2

0.4

0.6

0.8

1

P(Pa)

100009000800070006000500040003000200010000

Pr♦s t♠s♠ tc0 = 100m.s−1

X(m)

Z(m

)

0 0.10

0.2

0.4

0.6

0.8

1

P(Pa)

100009000800070006000500040003000200010000

t♠s♠ tc0 = 20m.s−1

r ♦♠♣rs♦♥ ♦ t ♣rssr ♥ t tr ♣t ♥ ♣r♦♦♣♥ ♥♥ ♦♥ r♦♠ t t♦ rt ♦r t♦ r♥t t♠ s♠s tr ts♠ ♣②s t♠

♦r♠ ❬❪ s s②st♠t rr♦r ♦ t t♠ srt③t♦♥ ♦ t ♦♥t♥t②qt♦♥ s ♥sr

♥② ♦tr ♥trt♦♥ t♠ s♠s ♥ ♦♥sr s s ♣r♦t♠ s♠ ♦ r t rr♦rs ♥ t ♥trt♦♥ ♦ t ♦♥t♥t②qt♦♥ ♦ ♠ ♥ t ♣rs♥t ♦r s t♦ ♦♥sr ♥ ♣♣r♦ tts t ♥st② ①♣t② s ♥t♦♥ ♦ t ♣rts ♣♦st♦♥s s s ♠♦r r♦st ♣♣r♦ s♣② tr s r♣s ♦r ♥t♦♥ ♦ t♣rssr ♥ ♥ ♦ t ♥st② ♥ ♦♠♣rss ♦s

♦♠♣t② ♣♦st♦♥♣♥♥t ② t♦ ♦♠♣t t ♥st②

rtr♥ t♦ t ♠♥ ♦ ♦rrt♥ t ♥♦♠♣t r♥ s♣♣♦rt ♥ s tt t ♦rrt ♦♥t♥t② qt♦♥ ♦♠s r♦♠

d (γaρa)

dt=

d

dt

(∑

b∈Fmbwab

)

γa

dρa

dt+ ρa

dγa

dt=

b∈Fmb∇wab.uab

♥ s♠r ② ❱ ❬❪ stt tt t ♦♥t♥t② qt♦♥ s strt②

q♥t t♦dρa

dt=

d

dt

(∑

b∈Fmbwab

) t♠ s ♦♥sr ♦♥t♥♦s r

qt♦♥ s s ② t♦ ♥trt ①t② ♥ t♠ t q♥tt② γaρa

t ♣rts ♣♦st♦♥s ♠♦ r♦♠ rnb t♦

rn+1

b

s ♣r♥ts s②st♠t

t♠ ♥trt♦♥ rr♦rs ♥ ♠s ρna ♣♥ ♦♥② ♦♥ t ♣♦st♦♥s ♦ ♣rts

Page 15: Unified semi-analytical wall boundary conditions for ...

t t s♠ t♠ ts ♣r♦♣rt② t♦tr t s♠♣t t♠st♣♣♥ ♥srst ♦♥srt♦♥ ♦ ♥ ♥r② s ❬❪ ♦r ts

s s t♦ t ♦♦♥ t♠ ♥trt♦♥ s♠

un+1a =un

a − δt

ρna

Gradn

apnb + g

rn+1a = rn

a + δtun+1a

(γaρa)n+1

=(γaρa)n

+∑

b∈Fmb

(wn+1

ab − wnab

)

r s♦s t rst ♦t♥ ② r♥ t t♠st♣ ♥ ♥t s②st♠t rr♦r ♥ t ♥st② qt♦♥ ♥ t t♠ s♠ t trst ♦t♥ t t t♠s♠ t rr t♠ st♣ ② ♦♥s♦ s♠ ♦ s ♦r t♦ st ♥ t♦ ♦♥r t t s r tt ♦st ♥st② r♥ t stst♦♥ t♠ t tr ♣t s rss rs t s ♥♦t t s ♦♥ t r t t ♥ s♠

♥t③t♦♥ ♦ t ♥st② t♠s♠ rqrs ♥ts ♦r t ♥st② ♥② ♦s r ♣♦ss rst ♦ ♣rt a♥ t rr♥ ♥st② ρ0 s ♥t

ρ0a = ρ0

s s ♦♥ ♣r♦s② t t ♦♥t♥t② qt♦♥ ♦ ♥ts tt t ♦♥t♥t② qt♦♥ ♦♥② ♠srs t rt♦♥ ♦ ♥st② ♥ ♥♦tt ♥t s♦rr ♦ t ♣rts ♦r t ♠♥ r s ♥ ♥♦♠♦♥t② t♥ ♣rts ♦ t♦ ♥♦♥♣②s ♦r s s ♣rts♦r♥② t t rsr rt♥ r♦♥ ♦ r♣s♦♥ ♥ srr♦♥ ②♦trs tr ♥ t s♠t♦♥ ♥ t ♥t ♥st②

ρ0

a

s ♥t③

♦r♥ t♦

ρ0a =

1

γ0a

b∈F0

mbw0ab

s ♥t③t♦♥ s t ♥t t♦ ♠♥t♥ ♦♠♦♥t② t♥ ♣rtst t♥ rqrs rsr ♦rrt♦♥

rsr ♦rrt♦♥ γ ♦rrt♦♥ ♣rs♥t s♦ r ♦s ♥♦t t

♥t♦ ♦♥t ♥② rsr ♦rrt♦♥ r ρa ≡∑

b∈Fmbwab ♣♥s

♦♥② ♦♥ t ♣rts ♣♦st♦♥s s s ♦r ♦♥srt♦♥ ♣r♦♣rts ♣r♦♠ s tt ρa ♠srs t♦ r♥t q♥tts

t r♥ ♦ t ♣rts s q♥tt② ♦ ♥trst ♥

t ♣rs♥ ♦ ♦s t♥ t r♥ s♣♣♦rt ♦ ♣rt

❲ r t t♠ st♣ ② stt♥ t s♣ ♦ s♦♥ t 100m.s−1 ♥st ♦20m.s−1

Page 16: Unified semi-analytical wall boundary conditions for ...

t s rqr tt t ♦ s ♦rrt t γa ♥①t t♦ t ♥♦t ♥①tt♦ t rsr ♦ ts s t ♦♦♥ ♣r tr ♥②

α (r) =∑

b∈F

mb

ρb

w (r − rb)

s♦ tt ♦r ♣rt a ∈ F \ E

αa ≡∑

b∈F

mb

ρb

wab

♦r ♥ ♣rt e ∈ E ♥ ♦r t ♠ ♦ s♠♥t s ∈ S t♦ r♥t♥t♦♥s ♦ α r s

αe ≡∑

b∈F\E

mb

ρb

web

s♥ αe s s t♦ t q♥tts s s t ♥st② ♦r t ♣rssr tt ♥ ♦s♥ ♥♦t t♦ t ♥t♦ ♦♥t ♣rts ♥ ♥tr♣♦t♦♥ s♥ ♦♥② t ♣rts ♦ t ♣②s q♥tts s st ♥st② ρ ♦r t ♣rssr p t t s s ➓

♠ s t♦ ♣♣② t ♣r tr ♦♥ t ♥st② t t♠st♣ t ♦♥② ♥①t t♦ t rsr s tt t ♥st② s ♥♦t ♦rrtr②r t αa s ♥ t ♥t② ♦ rsr tr s ♦♥t♥♦s♠① t♦ ♦rrt t ♦♥t♥t② qt♦♥

ρa [βγa + (1 − β) αa] = ρa =∑

b∈Fmbwab

r

β = exp

[−K

(min

αa

γa

; 1

− 1

)2]

♥ K s t♥ t♦ ♥ rtrr② ♦ − ln(0.05)

0.012≃ 30000 s♦ tt

β ≤ 0.05 ♥ αa

γa

≤ 0.99 ♦t β s ♥ t sr♠rr ♥s t ts s ♠♦st ♦♥ rs t t♥s t♦ ③r♦ s ♣♣r♦ t rsr

♦♠♣tt♦♥ ♦ t r♥♦r♠③t♦♥ tr♠s

♦r♠ ♥t♦♥s ♦ t ♦♠tr q♥tts γa ♥ ∇γa ♦r ♣rta r

γa ≡∫

Ω∩Ωa

w (r − ra) dr

∇γa ≡∫

Ω∩Ωa

∇aw (r − ra) dr =

∂Ω∩Ωa

w (r − ra)ndS

❲ r tt ∇γa r♣rs♥ts ♥ ♣♣r♦①♠t♦♥ ♦ t ♥♦r♠ t♦ t ♦r ♣rt ♦t t t ♣♦st♦♥ ra t ♣r♦s ♣♣r♦s s♥ ♣♦②♥♦♠♣♣r♦①♠t♦♥ ❬ ❪ ♥ ♥②t s♦t♦♥ ❬❪ ♥ srt s♠♠t♦♥ ♦r♦♥r② ♣♦♥ts ❬❪

Page 17: Unified semi-analytical wall boundary conditions for ...

s ♣♣r♦s ♥ts ♥ s♥ts sss rrr♥ ♦♠♣tt♦♥ ♦ t r♥♦r♠③t♦♥ tr♠ ♦ t r♥ s♣♣♦rt ♥r s♦ s ♦t♥ t t♠ ♥trt♦♥ s♠ tr② ♠♦r s②♦♥t♥ ♦r ♥② s♣ ♦ ♦♥rs ♣rs♥t ♥ ➓

♥②t ♦ ∇γa

❲t t ♦♥r② ♦ t ♦♠♥ ♦♠♣♦s ♦ s♠♥ts ♥♦t t t ssr♣t (.)s s♠♥t s ♥ ♥r ♥♦r♠ ns ♥♥♥ ♣♦♥t re1 ♥ ♥♥♥ ♣♦♥t re2 s r ♥ ♥ ♦♠♣t t ♥②t ♦ t ♦♥trt♦♥ ∇γas ♥ ②

∇γas ≡(∫

re2

re1

w (r) dl

)ns

r ♠ s♦♥ t ♥t♦♥s ♦ t ♦♠tr ♣r♠trs s t♦♦♠♣t t ♥②t ♦ ∇γas t

s ♦r t q♥t ❲♥♥ r♥ s ♥ ts ♦r

h

∫re2

re1

w (r) dl =(q2 cos α2)

πPq0

(q2) −(q1 cos α1)

πPq0

(q1)

+q40

π

(105

64+

35

512q20

)

sign (q2 cos α2) ln

(q2 + |q2 cos α2|

|q0|

)

−sign (q1 cos α1) ln

(q1 + |q1 cos α1|

|q0|

)

r t ♣♦②♥♦♠ ♥t♦♥ Pq0

s ♥ ②

Pq0(X) =

7

192X5 − 21

64X4 +

35

32X3 − 35

24X2 +

7

4

+q20

(35

768X3 − 7

16X2 +

105

64X − 35

12

)

+q40

(35

512X − 7

8

)

r q0 ≡ |raei.ns|h

qi ≡ |raei|h

♥ qi cos αi i ∈ 1, 2 r s♣② ♥ r

Page 18: Unified semi-analytical wall boundary conditions for ...

s ♥②t s ♥ st♠ts ♦ t rr♦r t♦ t ♣♣r♦①♠t♦♥s ♥ r ♦♠♣r t ♥②t ♥ ♣♣r♦①♠t s ♦ ∇γa

♥st t st♥ t♦ ♣♥ srt ♣♣r♦①♠t♦♥ s s ♥②

∇γas ≃ wasSsns

r t s ss♠ tt t r♥ s ♦♥st♥t ♦♥ s♠♥t s

r♥ s s t q♥t r♥ s ❬❪ ♥ t rt♦δr

h= 2 r δr

s t ♥t st♥ t♥ t♦ ♣rts ♥ h s t s♠♦♦t♥ ♥t s♦t rr♦rs r ♥ s

ǫ∇γa=

∣∣∇γ♥②ta −∇γsrt

a

∣∣∇γ♥②t

a

❲ ♦♥sr ♦♥② t ♦♠♣♦♥♥t ♦ ∇γa ♦rt♦♦♥ t♦ t ♥ r t rr♦r ♦r t srt③t♦♥ ♦ ∇γa s r② ♦♦ ♦r s ♣♦♦r srt③

t♦♥ rt♦δr

h♦r ♣♥ ss t♥ 0.1% rs t srt③t♦♥ s

s②st♠t rr♦r ♦r t ♣♣r♦①♠t♦♥ ♦ t ♦ γa ♦♥ t ♦rr ♦ 3%

❱s ♦ t ∇γa ♥t♦♥ ♥st t st♥ ♦t

❱s ♦ t rr♦r ♥t♦♥ ǫ∇γa♥st t s

t♥ ♦ t

r ♥②t ♥ r ♥ ♦♠♣t s ♥ r♥ ♦ t ♥t♦♥s ♥stt st♥ t♦ ♣♥

t srt③t♦♥ rr♦r ♦ ∇γa ♥ t ♣rs♥ ♦ ♦♠♣① ♦♥r②s s t s ♦♥ tt t rr♦r s rr ♦r♦r t rr♦r ss②st♠t s♦ tt t ♠♥t ♦ ∇γa s ②s ♥rst♠t ❲t♥ s♠t♦♥ ts s t♦ ♥♦♥♣②s ♦r ♣rts s t♦rs♦♥ ♦♥r② s♥ t rt② s ♥♦t ♥ ♦♠♣t② ② t r♣s ♦r ♣r♦♣♦rt♦♥ t♦ ∇γa

Page 19: Unified semi-analytical wall boundary conditions for ...

♦r♥♥ qt♦♥ ♦r γa

r♥ ♠t♦ t♦ ♦♠♣t γa ♦r ♣rt a ♥r s♦ ♦♥r② s sst t♦t t ♥ ♦r tt♦s ♣rts ♥ s tr♦r s♠♣r t♥ ♥♥②t ♦♠♣tt♦♥ ♠♥ ♦ t ♣rs♥t ♠t♦ s t♦ s ♦r♥♥qt♦♥ ♦ γa

dγa

dt= ∇γa.ua

γa = 1 ∂Ω ∩ Ωa = ∅

r t ♥t♦♥ ♦ t r♥t s ♦♠♥ t t t ttdra

dt= ua

♥♦tr ② t♦ ♦♥sr ts qt♦♥ s t♦ r♠r tt s q♥t t♦

∂γa

∂t= 0

γa = 1 ∂Ω ∩ Ωa = ∅

s ♠♥s tt t γa ♦s ♥♦t ♣♥ ♦♥ t t♠ t ♦♥② ♦♥ ♣♦st♦♥♥ s tr♦r ♥ r♥ s t s s ♠♥s t♦ ♦♠♣t γa t♦ ♦r♥t t ∇γa s sr t♦ ♦♠♣t s♥ t ♥ ①♣rss s sr ♥tr

rt♦♥ ♥ ①t♥ ♦r ♠♦♥ ♦♥rs ♥ t♦♥r② ♥ ② r ♠♦♥ ♦r♠ ♥ ts♥s tt s♠♥t ♦r tr♥ ♦♠♣♦s♥ t s ♠♦♥ t ts ♦t② t ♦♦♥ ♦r♠ s ♦t♥

dγa

dt=

s∈S∇γas.u

Rs

a

γa = 1 ∂Ω ∩ Ωa = ∅

r uRs

a s t ♦t② ♦ t ♣rt a ♥ rr♥ r♠ Rs r ts♠♥t s s ① γa s ♥♦ ♦♠♣t ② s♦♥ t ♦ qt♦♥s ♦♥ t ♥♦ ♦ ∇γas ♦♠♣t r♦♠

♥t③t♦♥ ♦ t γa

♥t③t♦♥ st♣ ♦ γ0a s ♦♥ ② ♠♥ rt tr♥s♦r♠t♦♥ ♦r

♣rt ♥t② ♥①t t♦ s♦ rtr♦♥ s∣∣∇γ0

a

∣∣ > 0 ♠♦t r♦♠ ts strt♥ ♣♦st♦♥ r0

a t♦ ♥ r r t ♥t♦♥ γ (r) ≡ 1 ♦r♥st♥

ra = r0a + l

∇γ0a

|∇γ0a|

r t ♥t l s t♥ t♦ 2R R s t rs ♦ t ♦♠♣t r♥s♣♣♦rt

st ♦ t ♣r♦♣♦s ♠t♦ s s♣② ♥ r ♦r ①♠♣ tr ♣rt ♥ r s ♣ ♥ t s ♥ r t ♦

t ♦s ♥♦t ♠♦

Page 20: Unified semi-analytical wall boundary conditions for ...

γ s 1 ♥ s ♠♦ t♦ ts ♥t ♣♦st♦♥ ♦♥ t ♣t ♦ t r rr♦ ♣t♥ t ♦ γa t rs♣t t♦ t ♦r♥♥ qt♦♥

0.82 0.84 0.86 0.88

0

0.01

0.02

0.03

0.04

0.05

10.950.90.850.80.750.70.650.60.550.5

γa

γ (r) = 1

γ (r) < 1

r t ♦ t ♥t③t♦♥ ♦ t γ ♥①t t♦ s♦

♦t tt t qt♦♥ ♦ γa s ♥trt ♥ t♠ t s♦♥♦rr t♠♥trt♦♥ s♠ t♦ ♣r♥t s②st♠t ♥trt♦♥ rr♦rs s ➓ ♥t♦

γn+1

a = γna +

1

2

(∇

nγa + ∇n+1γa

).(rn+1

a − rna

)

t s♦ ♦♥r② s ♠♦t♦♥ss ♥r ♦r♠ ♦r ♠♦♥ ♦r♠ s

γn+1

a = γna +

δt

2

s∈S

(∇

nγas + ∇n+1γas

).(uRs

a

)n+1

♦♥t♦♥ ♦♥ t t♠ st♣ s rqr t♦ ♣ t ♥trt♦♥ ♦ γa st

δt ≤ Ct,γ

1

maxa∈F ; s∈S

∣∣∣∇nγas.(uRs

a

)n∣∣∣

r Ct,γ = 0.005 r♦♠ ♥♠r ①♣r♥ s s ♥tr ♦♥t♦♥ ♥t s♥s tt t t♠ st♣ rss ♥ ♣rts ♣♦sss st ♦t② ♥♣♣r♦♥ ♦♥r② s s s♣s♥ ♥st ttr ♦♥t♦♥s ♦♥sr ♥ t♦♥ t♦ t s t♠st♣♣♥ ♦♥t♦♥s ♥ P

s ❬❪

♠r rsts

♠♥r ♥♥ ♦ tst s

♦ tst t rt♦♥ tr♠s ♥ t t sr strss ♦r♠t♦♥ ♠♥rP♦s ♦ ♥ ♦s♥♥ t ♣r♦ ♦♣♥ ♦♥rs s s♠t ♥♥ s ♠tr ♦ 1m t s♦st② ν s st t 10−1m2.s−1

s♦ tt t ②♥♦s ♥♠r s 10 s♦s tr♠ s ♠♦ t t♦rrt ♠♦ ♦ ♦rrs ♦♠♥ t t♦ ♦♠♣t t rt♦♥♦t② r s♦s tt t ♦r③♦♥t ♦t② ♣r♦ s ♥ ♦♦ r♠♥t t t ♥②t s♦t♦♥ ♥ ♥ t ♥t② ♦ t ts♠♦♥strt♥ tt t sr strss ♦rrt② ♥s t ♦② ♦r

Page 21: Unified semi-analytical wall boundary conditions for ...

0 0.2 0.4 0.6 0.8 10

0.2

0.4

0.6

0.8

1

0 0.20

0.2

0.4

0.6

0.8

1

10.90.80.70.60.50.40.30.20.10

ux

uxz

(m)

r P♦s ♦ ♥ ♣r♦ ♣♣ t ②♥♦s ♥♠r ♦ 10♦♦r ♦ts r♣rs♥t t ♦t② ♦ ♣rts t t st② stt rs t ♦ts • r t ♥②t ♣r♦

♦♠♣tt♦♥ ♦ t str♥ ♠♥r s ♦s s t♦ t ♦r♠ s♥ tr s ♥♦ ♥♥ ♦ t str♥ rt ♦♥ t ♦ ts s ts♦st② s ♦♥st♥t s s tst s ♦s s t♦ ♦♠♣r t ♦ t ♦♠♣t str♥ rt t♦ ts ♥②t ♥②t ♣r♦ ♦♦t② s

ux (z) = 4 Reν z

D2

(1 − z

D

)

s t♦ t ♦♦♥ ♥②t ♦ S

S (z) = 4 Reν

D2

∣∣∣2 z

D− 1∣∣∣

S(s-1)

Z(m

)

0 1 2 3 40

0.2

0.4

0.6

0.8

1

t♥r ♠♦

S(s-1)

Z(m

)

0 1 2 3 40

0.2

0.4

0.6

0.8

1

♦rrt♦♥ ♦ t♥r ♠♦

r ♦♠♣rs♦♥ ♦ t str♥ rt ♦r r♥t ♠♦s ♥ ♠♥r ♥♥♦

❲ ♥♦t ♥ r tt ♥ ts t♦rt tst s t ♦rrt ♠t♦

Page 22: Unified semi-analytical wall boundary conditions for ...

s stst♦r② r♣r♦t♦♥ ♦ t sr strss ♥①t t♦ t ♥t ♣r♦s ♠t♦s

t tr ♥ ♠ r ♥ t♥ t

♥ ts st♦♥ t ♣r♦♣♦s s♠ s tst ♦♥ ♠♦r ♦♠♣① ♦♠tr② ♦♥ssts ♦ s♥ ♦ ♣♣r♦①♠t② 2m ♥t ♥ 1m t t

♦ π2

rad ♥ ♥√

28

m ♦ t ♥ t ♦tt♦♠ ♠ ♦ t t♥ s♦♠tr② s ♦s♥ s♣② s♥ t trs ♦t s♦♥t♥♦s♣♦♥t ♥ s♦♣♥ ♣r♦ tsts t ♦rrt♦♥ ♦ t r♥ ♥ t ♣rs♥♦ rt② ♦♠♣rs♦♥ s ♠ t♥ r♥t ♠♦s ♥ st tr s♥ ②♥♠ s r t s♦st② ν s st t 10−2m2.s−1

t tr s

♦♠ trt♠♥ts ♦r s♦ ♦♥rs sr r♦♠ ♥ ♥t② t♦ r♣r♦ ♦rrt② st tr s r ♦♠♣r t rsts ♦t♥ ♥ t s♥s t 0.5m ♦ tr ♦r tr ss t ♥♥r♦♥s r♣s ♦rss ❬❪ t tt♦s ♣rts ♠t♦ s ❬❪ ♥ t♥ ♥ ♣r♦♣♦s ♠t♦s ①♣t t r♣s ♦rs ♣r♦ ♣♦♦r rsts s t rs ♥ t s♥s tt ♣rts ♣ s♥ ♦♥ rt t s t♦ tt tt t ♠ss♥ r ♥ t r♥ s♣♣♦rt s ♥♦t ♦♠♣♥st ♥ tst rt② s ♥♦t ♥ s♥t② ♣♦t ♦ t ♣rssr ♦ ♣rts♥st t ♣t s tr♦r ♥♦s② ♥ ② r♣r♦ ♥①t t♦ t ♦tt♦♠ tt♦s ♣rts ♠t♦ s r s ttr rsts t t♦♥t♦♥ s ♥♦t ♥sr ♥ s♦ t ♣rssr ♣r♦ s st ♥♦s② ♦r♦rts ♣♣r♦ s ♣r♦♠t t♦ sr ♥ ♦♠♣① ♦♠trs ♥ rqrst ♣rts t♦ ♠♠ t ♦♥r② ♥rs t ♦♠♣tt♦♥ ♦st ♣rs♥t ♠t♦ s s♣r♦r rsts ♥r ♣rssr ♣r♦ ♥ ♥rt ♦tt♦♠ ♥ ③r♦ ♦t② s s♦♥ ♥ r

②♥♠ s

s♠t♦♥ ♦ ♠ r t t s♠ ♦♠tr② s ♥ ♣r♦r♠ ♦r tt♦ ♦♥r② t♥qs ♣r♦s② sr ♥ t ♣rs♥t ♦♥ trs ♥t② ♦♠♥ ♦ 1m t ♥ 0.5m t ♦♥ t t♥ s ♦ ts♥ ♥ t rsts s♦♥ ♥ r ♣♣r♦s ♥sr ♠♣r♠♦♥rs t ♦t ♦ r♣s ♦rs ♠t♦ ♥ tt♦s ♣rts ♠t♦ ♥♦sr ♣rssr rtr♠♦r s♠t♦♥ t ♥r rs♦t♦♥s ♥ ♦♠♣t ② ♦♥ rs♦t♦♥ ♥ ♥ t ♥♠r ♦ ♣rts♥♣s♦ts ♦ t ♣rssr t t s♠ ♣②s t♠ r ♣♦tt ♦♥ tr

♦♠♣rs♦♥ t ❱ s♠t♦♥ ♦♥ t ♥t ❱♦♠ ♦♣♥s♦r ♦ ♣♥♦♠ ♦ t ♣rssr ♦♥ t t s ♦ t s ♣r♦♠♥ s♣② ♦♥ r

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tt♦s ♣rts

♥♥r♦♥s t②♣ r♣s ♦r

Prs♥t ♠t♦

r ♦♠♣rs♦♥ ♦ t rt ♦t② ♦r st tr ♥ t♥ t ♦r r♥t ♦♥r② ♦♥t♦♥s tr 20s

♦♠♣rs♦♥ ♦ t k − ǫ ♠♦ t P ♥ ♥t

❱♦♠s s♠t♦♥ ♦ s ♣ss

♥ ♠ s t ♦♥ rr t ♦♥t♥t② ♦ t ♦ s sr♣t ♥ t♠rt♦♥ ♦ s s ♥trr♣t ♦r s♣s s s s♦♠ s♠♦♥ t ②rqrs t ss t♦ ♠rt r ♣rr ♦ rst♦r t ♠rt♦♥ ♣r♦sss ♣sss r ♥st ♦♥sst ♦ ♠♥② r♣t♥ ♠♥ts ♥ ♥ ♦♥sr s ♣r♦ ♦ ♠♥s♦♥♥ ♦ ts ♦♠♣♦♥♥ts rqrs t ♥♦ ♦ t tr♥t ♦ t♥ st♦♥ s♥ t s③ ♦t r s ts t t② ♦ t s t♦ s♠ ♣str♠

Page 24: Unified semi-analytical wall boundary conditions for ...

♥♥r ♥ ♦♥s r♣s ♦rs tt♦s ♣rts

Prs♥t ♠t♦ Prs♥t ♠t♦ t t s♠rs♣ srt③t♦♥

r ♦♠♣rs♦♥ ♦ t ♣rssr ♦r ♠ r tst s ♥ t♥t ♦r r♥t ♦♥r② ♦♥t♦♥s

0500100015002000

0 0.5 1 1.5 2Pressurefor e(N)

Time (s)

VOF 7 × 103 ellsVOF 3 × 104 ellsVOF 1 × 106 ellsSPH 5 × 10

3 parti lesSPH 2 × 104 parti lesSPH 8 × 104 parti les

r ♦♠♣rs♦♥ ♦ t t♠ ♦t♦♥ ♦ t ♣rssr ♦♥ t t s♦ t t♥ t ♣rs♥t P ♦r♠t♦♥ ♥ t ♥t ♦♠ ♦♣♥♦♠ t r♥t s♣ srt③t♦♥

t♦ t ♦r ♦ t ♦ t♦ s ♣ss s 3D rsr♦ ♦♥sr r 2D s♠t♦♥s r t rt rt♦♥ r ss♠t♦ ♥ ❲ r♣t r t s♠t♦♥s ♣rs♥t ♥ ❱♦ t ❬❪ ♦♠tr② ♦ t x−♣r♦ s♠t♦♥ s ♣rs♥t ♥ r rsts ♦t♥ ② P r ♦♠♣r t♦ s♠t♦♥s ♦♥ t ♦❴tr♥ ② t ♥t ❱♦♠ ♦ ♦♣ ② s ❬❪ ♠ ♦ s ♦♠♣rs♦♥ s t♦ t t ♣r♦r♠♥ ♦ P ♦r tr♥ts♠t♦♥ ♦♠♣tt♦♥ s ♦♠♣r t② s♦♥ t s♠ qt♦♥s

Page 25: Unified semi-analytical wall boundary conditions for ...

t ②♥♦sr r t♦s t t k − ǫ ♠♦ t t s♠

♣rssr r♥t rs♣♦♥s r♥ t ♦ ∆p

ρ∆x= 1.885m.s−2 t t t♦

r♥t ♣♣r♦s r♥♥ ♥ r♥ t t♦ r♥t srt③t♦♥♣♣r♦s P ♥ ♥t ❱♦♠

♦t② ♣r♦s t ♦t♦♥s P1 P2 ♥ P3 ♥ ♥ r r♣♦tt ♥ r rsts s♦ tt t ♠ss ♦ s ♣r♦s♦s t♦ t ♦♥s ♦t♥ t t ♣rs♥t P s♠ t s♦ ♥♦t ttt t st♥r P ♠t♦ ❬❪ t ♣rt ♦t② ♥ ② s♦st②strt♦♥s ♥♦t t t ♥t ❱♦♠ ♦♥s ❲t t ♣rs♥t ♠♦ ♦♥♥ s tt t r♠♥t s r② stst♦r②

♦♥s♦♥

♣rs♥t rt s ♣rs♥t ♥ ♣♣r♦ t♦ t s♦ ♦♥r②♦♥t♦♥ s ♦t s♠♣ ♥ r♦st s♠♣t② s ♥ t ♠♥♥r ♦♠♣t t r♥ r♥♦r♠③t♦♥ tr♠ γa t ♥trt♦♥ ♥ t♠ ♦♥② rqrs t ♦♠♣tt♦♥ ♦ ts r♥t ∇γa r♦st♥ss s t♦ t ♥trt♦♥ ♥ t♠ ♦ t ♦♥t♥t② qt♦♥ ♠s t ♥st② ♣♥ ♦♥② ♦♥ t ♣rts ♣♦st♦♥s s ♦s ♦♥ t♠ s♠t♦♥t rt② r t♠ st♣ ♥ s ♠♦r ♥t ♦r ♦♥srt♦♥♣r♦♣rts

♥t♦♥ ♦ ♥ ♦♥r② ♦rrt r♥t ♥ ♣♥ ♦♣rt♦rss s t ♦♣♣♦rt♥t② t♦ ① ♦♥r② ♦♥t♦♥s ♥ ①s ♦♥ t ♣rssr t sr strss ♥ ♥ t sr s s s k ♥ ǫ ♥ ♠♦♦ tr♥

♦r ♥♠r♦s sss st rqr ♥stt♦♥ ♥ ♦♣♠♥t ♥♠②

❱t t ♣rs♥t ♦r♠t♦♥ ♦♥ r♥t tst s s s ♣r♦tr♥t ♠♣

♣t t r♥♦r♠③t♦♥ t♦ 3D t ♠♥ ♥ s t♦ ♥ ♥♥②t ♦r♠ ♦r t ♦♠♣tt♦♥ ♦ t ♦♥trt♦♥ ♦ sr♠♥t s ♦r t ♦ ∇γa ♦ ♣rt a s ♥♦t ②∇γas ♦r ② t♦ ♦♠♣t rt② ♥ ♣♣r♦①♠t ♦ t

t② t t♦rt ♦♥srt♦♥ ♦r ♥♦♥♦♥srt♦♥ ♦ ♠♦♠♥t♠♥ ♥r ♠♦♠♥t♠ ♥ s♣② ♥ ♣r♦ ss

♦♠♥ t ♣rs♥t ♣♣r♦ t ♥♦♥♣r♦ ♥tr♥ ♦♥t♦♥s

r♥t ♦♥t♦♥s ♥ P

♦♠♣tt♦♥ ♦ t rt♦♥ ♦t② ♥ tr♥t

s

❲ ♥ ♣♣② t s♠ ♦rrt♦♥ ♦ t s♦♥ tr♠ ♦ t ♠♦♠♥t♠qt♦♥ s t ♠♥r ♦♥ ♥♦t♥ tt (µ + µT )S.n ≃ ρuτuτ ♥ t ♥t②

Page 26: Unified semi-analytical wall boundary conditions for ...

♥t ♦ t ♦t② tP❯

r♥t s♦st② νT t ♦❴tr♥

r♥t s♦st② νT t P❯

r♥t s♦st② νT t ♦❴tr♥

♥t ♥r② k t P❯ ♥t ♥r② k t ♦❴tr♥

r ♦♠♣rs♦♥ ♦ t k − ǫ ♠♦ t r♥♥ P ♣♣r♦♥ ♥ r♥ ♥t ❱♦♠ ♠t♦ ♥ s♠t s ♣ss

♦ ❯♥ t qt♦♥ ♥s rt♦♥ ♦t② t♦ t ♠♥♦t② ♥ t tr♥t s ♥ ♥♦tr ♥t♦♥ s♦st② s♥♦t ♦♥st♥t ♥②♠♦r ♥ s s♣♣♦s t♦ ♥r ♥ t ♥t② ♦ ♥ t ♥ s♦♥ tt t ♦t② ♣r♦ ♥ tt r s ♦rt♠s♣ ts ③♦♥ s t ♦ ②r ♦♥sr t ♣rt a t♦ ♥

♦r♠② t k = 0 ♥ t♥ νT = 0 s♦ tt r♦r t ♠♥r s ♦rt s♦s s②r r t ♠♥r s♦st② s ♠♦r ♠♣♦rt♥t t♥ t tr♥t ♦♥ ss② ♦r ♥r♦♥♠♥t ♦s r② t♥ s♦ tt ♦ ♥♦t ♥♦r k t♦ ③r♦ t

♥ ♥♥ ♦ ts ss♠♣t♦♥ s r ♥ 10% ♦ t ♥♥ ♣t

Page 27: Unified semi-analytical wall boundary conditions for ...

Pr♦s ♥ P1 Pr♦s ♥ P2 Pr♦s ♥ P3

r Pr♦s ♦ t ♦t② ♠♥t ♥ tr r♥t ♣♥s ♥ t s♣ss k − ǫ ♠♦ ♥ r ♥ t k − ǫ ♠♦ t ♦❴tr♥ ♥r♥

t ♦ ②r ♦ s♠♦♦t uτ ♥ ♦t♥ r♦♠ t ♦♦♥ t ♥ trt ♦rt♠

|ua|uτa

=1

κln(zauτa

ν

)+ 5.2

♦ qt♦♥ ♠st r② tt t ♥♦♥♠♥s♦♥ st♥ t♦ t zauτa

νs rtr t♥ 11 ❲ ♦ s♦ s ♦ s ♦r r♦ s ♦r s

s ♦ ♦t ♥ t ♠♥r ♥ t ♦ ②r s s rs t t♥ t k − ǫ ♠♦ ♠st s♦ ♠♦ ♦r ♦ ②♥♦s ts♦r ♠♦r ♥♦r♠t♦♥ s ❬❪

❱♦t② t t

❲ ♦sr ♥ t ♦r♠ tt t ♦t② t t us s ♦♥sr♥ t ♦♥r② tr♠ ♦r♠② t ♥♦s♣ ♦♥t♦♥ ♦ ♠♣♦s tt t♦t② t t s t ♦t② ♦ t ts 0 ♦r ♠♦t♦♥ss s s ♠♣♦s ♦r ♠♥r ♦ ♥ t tr♥t s t s ♣rr t♦ ♥♦t♦ s♦ t s♦♣ ♦ t ♦t② ♣r♦ s ♠ rr t t t♥ ♥ t♦ ②r r ♣rts r ss♠ t♦ s ♥t t♦ trt② Sa ♥①t t♦ t ♥ t♦ ♥tr♣♦t t ♦t② t t ♦ ♦ s♦ t t ♦t② ue ♦ ♣rts ♥ t s♦s ♥ rt♦♥tr♠s

due

dt=

1

γe

b∈Fmb

µTe + µTb

ρeρb

ueb

r2eb

reb.∇web

︸ ︷︷ ︸s♦s tr♠

− 2uτeuτe

γe

s∈S|∇γes|

︸ ︷︷ ︸rt♦♥ tr♠

❲ ♥♦t r tt qt♦♥ s t ♠♦♠♥t♠ qt♦♥ ♣♣ t♦ ♥ ♣rt t ♥tr rt② ♥♦r ♣rssr r♥t ♥ ♥ us t♦ t r t♥ ♣rts e1 ♥ e2 ♥ ♥ ➓ stt t♦ ♦ ♥ ♦ s♣ ♦t② t t ♥ ②♥♦s ♥♠rs♠t♦♥ s s♦ s ♥ ♠♥② ♦s s s ♥ ♥t♠♥ts s r♦t ❬❪ ♥t② t♦ r ♥ ♠♥ tt t ♣rts ♥ E r ♥ t r♥ ♣♦♥ts ♥ ♦ ♥♦t ♠♦ t t ♦t② ue

t t t ♦t② t s t♦ s② ♦♥② s t ♦t② ue t♦ ♣ts♦s ♦rs ♦ ♣rts ♥trt♥ t t ♥ t♦ ♦♠♣t tstr♥ rt S

Page 28: Unified semi-analytical wall boundary conditions for ...

① ♦♥t♦♥s ♦♥ t ♥t ♥r②

♣♥ ♦♣rt♦r ♣♣ t♦ t tr♥t ♥t ♥r② rs t♦

1

ρa

Lapa

(µb +

µTb

σk

, kb)

=1

γa

b∈Fmb

2µ + µTa/σk + µTb/σk

ρaρb

kab

r2ab

rab.∇wab

s t s ss♠ tt tr s ♥♦ ① ♦ k r♦♠ t ♦♥r② ∂k

∂n=

0 t t qt♦♥ s♦ s ♥ ♣ ♦ Lapa ♥ ♣②s ♠♥♥ s tt t tr♥t ♥t ♥r② s ♦♥② rt ② t♠♥ ♦ ♦r♦r ♥st ♦ s♣②♥ ♦♥r② ♦♥t♦♥s t t t ♥t♦♥ ♣♣r♦ srs t ♥ ♦ tr♠s ♥ t ♥t② ♦

t r t s ss♠ tt P = ǫ ts ♠♣s tt t ♦♥t♦♥∂k

∂n= 0

s ♥♦t ♦♥② t t t ♥ t ♦ ♥t② ♦ t s♦ ♦♥r② ss♠ t ♦ t♦ ② tr♥t tt s t♦ s② t t♥

s♦s s②r ♥ s ②♥♦s ♥♠r s ♦r k − ǫ ♥ t ♦ ♥♦t s♦ t k− ǫ ♠♦ ♣ t♦ t r k s t♦rt② ①♣t t♦ 0 t ♣ t♦ s♠ st♥ δ r♦♠ t r t tr♥ s ②sts νT ≫ ν ♠♥ ♥t ♦ t ♣rs♥t r♥♥ ♣♣r♦♦♠♣r t♦ ♥ r♥ ♦♥ s tt t r♥♥ ♣rts ♥ F \ E t st t st♥ ♦ t ♦rr ♦ δr r♦♠ ♥② t s ♦♥ ♦t ♠♥ ♥ts ♦♠♣r t♦ t ♠ss ♠t♦s r t ♦♥r②♠♥ts r s♣♣♦s t♦ t rt st♥ t♦ t t r ♦♥②♦s ♦♥ ♣rts r t② t ♥♦♥③r♦ st♥ r♦♠ t s

♦ st♠t k t t ♥ t s ♦r t ♥st② t♣rssr ♦r t sr strss

ke =1

αe

b∈F\EVbkbwbe

❲ ♥♦t tt ts ♣♣r♦①♠t♦♥ s ♦♥sst♥t t t ss♠♣t♦♥∂k

∂n= 0

♥②

ks =ke1 + ke2

2

① ♦♥t♦♥s ♦♥ t ss♣t♦♥ ♦ ♥t ♥r②

♣♥ ♦♣rt♦r ♣♣ t♦ ǫ rqrs t ♦r ∂ǫ/∂n ♥♥ ss♠ tt t ♦ s ② tr♥t t♥ r② s♥ ♣rt♥ t r ♦ ♥♥ ♦ ∃s ∈ S/ |∇γas| > 0 s ♥ t ♦ ②rr

k ≃ u⋆2

√Cµ

ǫ =u⋆3

κz

νT = κu⋆z

t qt♦♥s ♥ r r♦♠ t qr♠ P = ǫ

Page 29: Unified semi-analytical wall boundary conditions for ...

r z s t st♥ t♦ t ♣rt a s ♥trt♥ t sr s stt z = max (ras.ns; δr) r δr s t ♣rt r ♥t s♣♥κ s t ❱♦♥ r♠♥ ♦♥st♥t t t ♦ 0.41 ♥ u⋆ s rt♦♥ ♦t②♠sr♥ t tr♥

u⋆s =

√ks

C1

4

µ

♥ r♦♠ qt♦♥ ♥ ♦r t ① ♦ ǫ

νTa

σǫ

∂ǫa

∂ns

= − 2u⋆4s

σǫκδras

t♦r 2 s ♣r♦ ② rst♦rr ♣♣r♦①♠t♦♥ t ① s tt t st♥ z

2 s r② s ♥ s♣② r s ǫ s s♣♣♦s

t♦ r② s 1zr z s t st♥ t♦ t

s t ♣♥ ♦♠s

1

ρa

Lapa

(µb +

µTb

σǫ

, ǫb)

=1

γa

b∈Fmb

2µ + µTa/σǫ + µTb/σǫ

ρaρb

ǫab

r2ab

rab.∇wab

+4

γaρa

∑s∈S |∇γas| ρs

u⋆4s

σǫκδras

s s ♥ ♣ ♦ Lapa ♥

r♥s

❬❪ sr♠ ♦♥t s ❲ Pr♦t rt♦♥ ♦r♠t♦♥s ♦♥tt ♦rt♠ ♦r r ♦♥rs ♥ t♦♠♥s♦♥ s♣ ♣♣t♦♥s

❬❪ r ♦r♥ ss♥r♥ rr♥t P ♥ ♠♣r♦ s♣ ♠t♦♦rs r ♦rr ♦♥r♥ ♦r♥ ♦ ♦♠♣tt♦♥ P②ss

❬❪ ♦♥♦ ♥♥t t t ♥♥ ♦ s♠♥②t ♣♣r♦ ♦r s♣ ♠♦♥ ♦ s♦ ♦♥rs4th P ♦rs♦♣ ♥ts r♥

❬❪ ♦♥♥ tr ♣ ♣rt ♦♥r② ♦rs ♦r rtrr② ♦♥rs ♦♠♣tr P②ss ♦♠♠♥t♦♥s

❬❪ r♦♥ ♦ r♦ ♦ ♠ ♥♠r ♥♠r s♠s ♦rt s♣ ♠t♦ ♣♣t♦♥ ♥ r sr ♦s ♥ ♣t♦♥ tr♥s 4th

P ♦rs♦♣ ♥ts r♥

❬❪ ♦③é ss♥r♥ ♦r♠ ① ♠t♦ t t ♦♥r② ♦r s♣ 4th P ♦rs♦♣ ♥ts r♥

❬❪ ♦♥♥ ♠t♥ r sr ♦s t P ♦r♥ ♦ ♦♠♣

tt♦♥ P②ss

Page 30: Unified semi-analytical wall boundary conditions for ...

❬❪ ❱♦ ss ♠r ♠♦♥ ♦ ♦♠♣① tr♥t rsr♦s t t s♣ ♠t♦ ♥ ♦r ♥tr♥t♦♥ ♦r♥ ♦r

♠r t♦s ♥ s ♦ ❯tt♣①♦♦r

❬❪ ❱ P ❲t ♣rt ♣r♦s tr♠♠t♦s♥①t tr♠ ♥ s♠♦♦t♣rt ②r♦②♥♠s t ♦s t ♣♣

❬❪ ♠♥ ♦♥t ②♥♠ r♥♠♥t ♥ ♦♥r② ♦♥tt ♦rs ♥s♣ t ♣♣t♦♥s ♥ ♦ ♣r♦♠s ♥t ♦r♥ ♦r ♠r

t♦s ♥ ♥♥r♥ sr t♦s ♥t♥s ♥ ♣♣t♦♥s

❬❪ ♦♥♥ ♠♦♦t ♣rt ②r♦②♥♠s ♥♥ r ♦ str♦♥

♦♠② ♥ str♦♣②ss

❬❪ ♦rrs P ♦① P ❩ ❨ ♦♥ ♦ r②♥♦s ♥♠r ♥♦♠♣rss♦s s♥ s♣ ♦r♥ ♦ ♦♠♣tt♦♥ P②ss

❬❪ ❱♦ ♥s ♦ ② ♦♠♣rss ♦s ♥ ts ♣♣t♦♥

t♦ t P ♠t♦ t♦ ♣s

❬❪ ♥r ♣♥ t♠t ♠♦s ♦ tr♥ ♦♥♦♥♠ Prss

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❬❪ ♦st♥ P♦♦ ♦ ♦♥srt♦♥ ♦ t ♠t♦♥♥ s♦♥❲s② ♥ r♥s♦ 3rdedition

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②♥♠s ♥ r♠♦②♥♠s t♥s r

❬❪ ❲♥♥ Ps ♣♦②♥♦♠ ♣♦st ♥t ♥ ♦♠♣t② s♣♣♦rt r ♥t♦♥s ♦ ♠♥♠ r ♥s ♥ ♦♠♣tt♦♥

t♠ts ♠r

❬❪ ❱♦ ss ♥♠♦ ♦r ♦rt ♦♥ s ♣ss t s♣ ♥ r♥ ♦s t ♥♥♦ tr♥t ♦sr Pr♦ IIIrd P ♥tr♥t♦♥ ❲♦rs♦♣ s♥♥ ss

❬❪ ♦❴tr♥ ♥t ❱♦♠ ♦ ♦r t ♦♠♣tt♦♥ ♦ r♥t

♥♦♠♣rss ♦s ♥str ♣♣t♦♥s ♦ ♥tr♥t♦♥ ♦r♥♦♥ ♥t ❱♦♠s

❬❪ P♦♣ r♥t ♦s ♠r ❯♥rst② Prss

❬❪ r♦t ②r♦②♥♠s ♦ r r ♦s ♦♥ t t

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